Data recording medium, recording/reproducing apparatus, manufacturing apparatus, and method for providing optimum position of mark start and end parts

ABSTRACT

An optical disc has a plurality of tracks for recording information represented as marks and spaces between the marks. The marks are formed by an optical beam modulated by a plurality of drive pulses ( 202 ) where a number of the drive pulses is determined according to a length of a mark part in the original signal to be recorded to the track. The optical disc has a control information recording area ( 2504 ) for storing a first pulse position Tu value indicative of rising edge of the first drive pulse for determining a start position of a mark to be recorded, and a last pulse position Td value indicative of falling edge of the last drive pulse for determining an end position of a mark to be recorded.

This is a divisional application of Ser. No. 09/352,211 filed Jul. 13,1999, now U.S. Pat. No. 6,188,656.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a recording method for recordingoptical data to a writable data recording medium, and to the structureof a data recording medium used by this method.

2. Description of the Related Art

Devices for recording and reproducing optical data, particularly digitaldata, to data recording media have been the subject of much developmentdue to the ability of such devices to store large volumes of data usingmedia of a given physical size.

The phase change optical disk is one type of recordable optical datarecording medium. To record to a phase change optical disk, the beamfrom a semiconductor laser is focused on the rotating disk to heat andmelt, that is, change the phase of, a recording film. The temperature ofthe recording film and the rate at which the film cools vary, forexample, according to the intensity of the optical beam.

When the intensity of the optical beam is high, the film cools rapidlyfrom a high temperature state, and the recording film is changed to anamorphous phase. When the optical beam is relatively weak, the recordingfilm cools gradually from a medium-high temperature state, and therecording film thus crystallizes. The resulting amorphous areas of therecording film are normally referred to as a “mark” and the crystallizedpart between consecutive marks is normally referred to as a “space.”These marks and spaces can be used to record two-value data, that is, 0s and 1 s.

It is also to be noted that laser power, when the optical beam intensityis high, is referred to as “peak power,” and laser power, when theoptical beam intensity is low, is referred to as “bias power.”

When reproducing data, a low power optical beam, that is, a light beamnot strong enough to produce a phase change in the recording film, isemitted to the disk, and the light reflected back from the disk is thendetected. In general, the reflectance of the amorphous phase marks islow, and the reflectance of crystal phase spaces is high. A reproductionsignal can therefore be obtained by detecting the difference in theamount of light reflected from the marks and spaces.

Mark position recording (or PPM recording) whereby information isrecorded using the location of marks of a constant length, and mark edgerecording (or PWM recording) whereby information is recorded using thelength of the marks and the length of spaces between marks, are twomethods of recording data to a phase change optical disk. The datarecording density of mark edge recording is generally the higher ofthese two methods.

The mark edge recording method also generally records longer markscompared with the constant mark length in mark position recording. Whena peak power laser beam is emitted to a phase change disk to record along mark, heat accumulation in the recording film produces marks thatare wider in the latter half of the mark as seen in the radialdirection, something like a teardrop shape. Such marks significantlydegrade signal quality, causing, for example, degraded signal linearityin the recorded signal, increased jitter during reproduction, markremnants that are left when the marks are overwritten by directoverwrite recording, and signal crosstalk between tracks duringreproduction.

Recording shorter marks and spaces is one means of increasing therecording density. A short space length, however, can result in thermalinterference. For example, heat at the trailing end of a recorded markis transferred through the following space, which can then contribute toa temperature increase at the beginning of the following mark. Heat atthe beginning end of one recorded mark can also transfer through thepreceding space and affect the cooling process at the end of thepreceding mark. A problem with thermal interference in conventionalrecording methods is that mark edge positions will vary, causing ahigher error rate during reproduction.

To address the above-noted problems, Japanese Unexamined PatentApplication Publication (kokai) 7-129959 (U.S. Pat. Nos. 5,490,126 and5,636,194) teach a method for recording marks by segmenting that part ofthe recording signal corresponding to a mark in mark edge recording intostart, middle, and end parts, the start and end parts each having aconstant pulse width and the middle containing pulses of a constantperiod. This recording signal is then used to rapidly switch the outputof a two-value laser.

With this method, the width of the middle part of a long mark issubstantially constant and does not spread because laser output isdriven with a constant period pulse current producing the minimum powerrequired for mark formation. An increase in jitter at the leading andtrailing edges of the mark can also be suppressed during directoverwrite recording because the laser beam is emitted with a constantpulse width at the leading and trailing ends of the mark.

It is also possible to detect whether marks, or spaces before and aftera mark, are long or short, and change the position at which the startand end parts of a mark are recorded according to the length of the markand the leading and trailing spaces. This makes it possible tocompensate during recording for peak shifts caused by thermalinterference whereby heat at the end of a recorded mark transfersthrough the following space and affects the heating process at thebeginning of the next mark, and heat at the beginning of a next recordedmark conversely travels back through the preceding space and affects thecooling process at the end of the preceding mark.

The publication Kokai 7-129959 does not, however, teach a method fordetermining the optimum positions of the start and end parts of a mark,nor does it teach a specific structure and basis for changing oradjusting the start and end edge positions.

If such an optimum method and structure are not defined, the reliabilityof optimized recording will be low. Furthermore, even if optimizedrecording is achieved, it will be at the expense of excessive time spentsearching for the optimum position and excessive circuit cost.

A method for changing the start and end edge positions of a mark basedon the data being recorded has been invented as a means of achievinghigh density data recording. A problem with this method, however, isthat the edge of a recorded mark can move due to thermal interference asdescribed above. This edge movement phenomenon is also highly dependentupon the disk structure and the composition of the recording film, andif either of these change even slightly, optimized recording cannot beachieved.

SUMMARY OF THE INVENTION

With consideration for the above described problems, an object of thepresent invention is therefore to provide a method for determining theoptimum position of mark start and mark end parts.

A further object of the present invention is to provide a data recordingmedium wherewith optimized recording is possible even with disks ofdifferent types, including disk structure and recording filmcomposition.

To achieve the above objects, a data recording medium according to thepresent invention has a plurality of tracks to which data is recorded bycontrolling the lengths of marks and spaces remaining betweenconsecutive marks. The marks are formed by changing the opticalcharacteristics of the recording film in the track recording surface.More specifically, a mark start position and mark end position arevaried according to an input signal so that playback signal jitter is apredetermined constant value or less, and one or both of these adjustedstart position and end position values, or a typical value therefor, andthe method for using these adjusted start position and end positionvalues, are prerecorded to a predetermined location on the datarecording medium.

In a data recording medium according to the present invention, the markstart position can be determined based on the length of the mark part ofa recording signal and the space part immediately preceding the markpart. The mark end position can be similarly determined from the lengthof a mark part and the immediately following space part of a recordingsignal.

A data recording medium according to a first aspect of the presentinvention having a plurality of tracks for recording informationrepresented as marks and spaces between the marks, the marks beingformed by emitting to a track in the data recording medium an opticalbeam modulated by one or a plurality of drive pulses where a number ofthe drive pulses is adjusted according to a length of a mark part in theoriginal signal to be recorded to the track, comprises: a data recordingarea for recording data, and a control information recording area forstoring at least one of a first pulse position Tu value for determininga start position of a mark to be recorded, and a last pulse position Tdvalue for determining an end position of a mark to be recorded.

It is therefore possible to achieve recording optimized for specificdifferences in disk structure and/or recording film composition byreproducing these adjustment values and using them to generate anoptimized recording signal from which the marks and spaces are formed.

A data recording medium according to a second aspect of the presentinvention more specifically determines the first pulse position Tu fromthe length of a mark part and the immediately preceding space part inthe original signal, and determines the last pulse position Td from thelength of a mark part and the immediately following space part in theoriginal signal.

It is therefore possible to compensate during recording for the effectsof heat accumulation and thermal interference during recording, and forequalizer distortion during reproduction, to achieve recording withlittle jitter.

A data recording medium according to a third aspect of the presentinvention yet further expresses the first pulse position Tu as a timedifference TF between a first reference point R1, which is a leadingedge of a mark part in the original signal to be recorded, and a firstedge of the first pulse in a plurality of drive pulses, and expressesthe last pulse position Td as a time difference TL between a secondreference point R2, which has a specific known position relative to atrailing edge of a mark part in the original signal to be recorded, anda trailing edge of the last pulse in a plurality of drive pulses.

It is therefore possible to obtain mark start position and mark endposition more accurately.

In a data recording medium according to a fourth aspect of the presentinvention, the length of mark parts in the original signal and thelength of space parts between the mark parts are further specificallyexpressed as a value NT where T is a reference period, and N is apositive integer from n1 to n2. Mark and space parts are furtherseparated into a plurality of groups used for mark start and endposition adjustment according to mark and space length; and specificfirst pulse position Tu and last pulse position Td values are set foreach adjustment group.

Circuit scale can therefore be reduced by combining a plurality of marklengths and space lengths into a single group. Recording with even lessjitter can also be achieved by reducing the number of mark lengths andspace lengths in the group as the mark and space length decreases, andthus increasing the number of groups as mark and space length decreases.

A data recording medium according to a fifth aspect of the presentinvention further specifically separates mark parts by length into threegroups, and separates space parts by length into three groups.

A data recording medium according to a sixth aspect of the presentinvention yet further separates mark parts by length into four groups,and separates space parts by length into four groups.

Recording with less jitter can thus be achieved by even more preciselyseparating mark and space lengths and further increasing the number ofadjustment groups.

A data recording medium according to a seventh aspect of the presentinvention increases the number of adjustment groups as a length of themark part and a length of the space part decreases.

Shorter marks and spaces occur more frequently, and by using a signalwith a high frequency of occurrence as the reference signal foradjusting mark position, it is possible to record with less jittercompared with using a signal with a low frequency of occurrence as thereference signal.

In a data recording medium according to an eighth aspect of the presentinvention n1 is 3 and n2 is 11.

In a data recording medium according to a ninth aspect of the presentinvention, mark parts are separated by length into three groups of 3T,4T, and 5T or longer marks, and space parts are separated by length intothree groups of 3T, 4T, and 5T or longer spaces.

In a data recording medium according to a tenth aspect of the presentinvention, mark parts are separated by length into four groups of 3T,4T, 5T, and 6T or longer marks, and space parts are separated by lengthinto three groups of 3T, 4T, 5T, and 6T or longer spaces.

In a data recording medium according to an eleventh aspect of thepresent invention, there are two or more methods of using Tu and Td witha plurality of pulses, and information indicative of the method of useis prerecorded to the control information recording area.

In a data recording medium according to a twelfth aspect of the presentinvention, the method of Tu use uses Tu to change the rising edgeposition of a first drive pulse without changing the width thereof, andthe method of Td use uses Td to change the falling edge position of alast drive pulse without changing the width thereof.

In a data recording medium according to a thirteenth aspect of thepresent invention, the method of Tu use uses Tu to change the width of afirst drive pulse without changing the falling edge position thereof,and the method of Td use uses Td to change the width of a last drivepulse without changing the rising edge position thereof.

In a data recording medium according to a fourteenth aspect of thepresent invention, the information indicative of the method of Tu and Tduse is recorded to a position before the position where the Tu and Tdvalues are recorded referenced to the direction in which information isrecorded.

A fifteenth aspect of the present invention relates to a method forobtaining a first pulse position Tu for a data recording medium having aplurality of tracks, marks formed by emitting to a track in the datarecording medium an optical beam modulated by one or a plurality ofdrive pulses where a number of the drive pulses is determined accordingto a length of a mark part in the original signal to be recorded to thetrack, a data recording area for recording information using the marksand spaces between the marks, and a control information recording areahaving recorded thereto at least a first pulse position Tu value and alast pulse position Td value whereby at least a first pulse position Tuand a last pulse position Td of the drive pulse is changed so as to makea reproduction jitter a specific value or less. This method comprises:generating a pattern signal containing a pattern of consecutive markparts with a specific length of PT and space parts with a specificlength of QT where T is a reference period, P is a positive integer fromn1 to n2, and Q is a positive integer from n1 to n2; storing the patternsignal; generating a plurality of drive pulses from the pattern signal;forming spaces and marks on the data recording medium by generating andemitting thereto an optical beam modulated according to the plurality ofdrive pulses; reproducing the marks and spaces recorded to the datarecording medium; comparing and obtaining a difference between acombination of mark and space parts in the reproduced reproductionsignal, and a combination of mark and space parts in the stored patternsignal; and obtaining from this difference a first pulse position Tu forapplication to an original signal containing a sequence of space partsof length QT and mark parts of length PT.

More specifically according to a sixteenth aspect of the presentinvention, first pulse position Tu is obtained for a plurality ofcombinations of mark lengths and space lengths by changing the values ofP and Q.

More specifically according to a seventeenth aspect of the presentinvention, the pattern signal contains an adjustment signal forobtaining a DSV of 0.

An eighteenth aspect of the present invention relates to a method forobtaining a last pulse position Td for a data recording medium having aplurality of tracks, marks formed by emitting to a track in the datarecording medium an optical beam modulated by one or a plurality ofdrive pulses where a number of the drive pulses is determined accordingto a length of a mark part in the original signal to be recorded to thetrack, and a control information recording area for recordinginformation using the marks and spaces between the marks, and havingrecorded thereto at least a first pulse position Tu value and a lastpulse position Td value whereby at least a first pulse position Tu and alast pulse position Td of the drive pulse is changed so as to make areproduction jitter a specific value or less. This method comprises:generating a pattern signal containing a pattern of consecutive markparts with a specific length of PT and space parts with a specificlength of QT where T is a reference period, P is a positive integer fromn1 to n2, and Q is a positive integer from n1 to n2; storing the patternsignal; generating a plurality of drive pulses from the pattern signal;forming spaces and marks on the data recording medium by generating andemitting thereto an optical beam modulated according to the plurality ofdrive pulses; reproducing the marks and spaces recorded to the datarecording medium; comparing and obtaining a difference between acombination of mark and space parts in the reproduced reproductionsignal, and a combination of mark and space parts in the stored patternsignal; and obtaining from this difference a last pulse position Td forapplication to an original signal containing a sequence of space partsof length QT and mark parts of length PT.

It is therefore possible to accurately obtain mark start position Tu andmark end position Td using simple specific patterns with a short patternlength.

Yet further preferably according to a nineteenth aspect of the presentinvention, this method obtains last pulse position Td for a plurality ofcombinations of mark lengths and space lengths by changing P and Q.

Yet further preferably according to a twentieth aspect of the presentinvention, this method uses a pattern signal containing an adjustmentsignal for obtaining a DSV of 0.

A twenty-first aspect of the present invention relates to an apparatusfor obtaining a first pulse position Tu for a data recording mediumhaving a plurality of tracks, marks formed by emitting to a track in thedata recording medium an optical beam modulated by one or a plurality ofdrive pulses where a number of the drive pulses is determined accordingto a length of a mark part in the original signal to be recorded to thetrack, and a control information recording area for recordinginformation using the marks and spaces between the marks, and havingrecorded thereto at least a first pulse position Tu value and a lastpulse position Td value whereby at least a first pulse position Tu and alast pulse position Td of the drive pulse is changed so as to make areproduction jitter a specific value or less. This apparatus comprises:means (125) for generating a pattern signal containing a pattern ofconsecutive mark parts with a specific length of PT and space parts witha specific length of QT where T is a reference period, P is a positiveinteger from n1 to n2, and Q is a positive integer from n1 to n2; means(120) for storing the pattern signal; means (111) for generating aplurality of drive pulses from the pattern signal; means (109, 103-106)for forming spaces and marks on the data recording medium by generatingand emitting thereto an optical beam modulated according to theplurality of drive pulses; means (105-108, 112-115) for reproducing themarks and spaces recorded to the data recording medium; means (120) forcomparing and obtaining a difference between a combination of mark andspace parts in the reproduced reproduction signal, and a combination ofmark and space parts in the stored pattern signal; and means (127) forobtaining from this difference a first pulse position Tu for an originalsignal containing a sequence of space parts of length QT and mark partsof length PT, and storing first pulse position Tu.

Further preferably according to a twenty-second aspect of the presentinvention, first pulse position Tu is obtained for a plurality ofcombinations of mark lengths and space lengths by changing P and Q.

Further preferably according to a twenty-third aspect of the presentinvention, the combinations are classified, and the reproducing meanscomprises an equalizer (114), and the ratio between the output amplitudeof the equalizer at the frequency of the longest mark and the outputamplitude of the equalizer at the frequency of the shortest mark is 3 dBor less, provided that the longest mark and the shortest mark are fromthe same classification.

Distortion error by the equalizer during reproduction can therefore bereduced, and recording with less jitter can be achieved.

Yet further preferably according to a twenty-fourth aspect of thepresent invention, the pattern signal contains an adjustment signal forobtaining a DSV of 0.

A twenty-fifth aspect of the present invention relates to an apparatusfor obtaining a last pulse position Td for a data recording mediumhaving a plurality of tracks, marks formed by emitting to a track in thedata recording medium an optical beam modulated by one or a plurality ofdrive pulses where a number of the drive pulses is determined accordingto a length of a mark part in the original signal to be recorded to thetrack, and a control information recording area for recordinginformation using the marks and spaces between the marks, and havingrecorded thereto at least a first pulse position Tu value and a lastpulse position Td value whereby at least a first pulse position Tu and alast pulse position Td of the drive pulse is changed so as to make areproduction jitter a specific value or less. This apparatus comprises:means (125) for generating a pattern signal containing a pattern ofconsecutive mark parts with a specific length of PT and space parts witha specific length of QT where T is a reference period, P is a positiveinteger from n1 to n2, and Q is a positive integer from n1 to n2; means(120) for storing the pattern signal; means (110) for generating aplurality of drive pulses from the pattern signal; means (109, 103-106)for forming spaces and marks on the data recording medium by generatingand emitting thereto an optical beam modulated according to theplurality of drive pulses; means (105-108, 112-115) for reproducing themarks and spaces recorded to the data recording medium; means (120) forcomparing and obtaining a difference between a combination of mark andspace parts in the reproduced reproduction signal, and a combination ofmark and space parts in the stored pattern signal; and means (127) forobtaining from this difference a last pulse position Td for an originalsignal containing a sequence of space parts of length QT and mark partsof length PT, and storing last pulse position Td.

Further preferably according to a twenty-sixth aspect of the presentinvention, first pulse position Tu is obtained for a plurality ofcombinations of mark lengths and space lengths by changing P and Q.

Further preferably according to a twenty-seventh aspect of the presentinvention, the combinations are classified, and the reproducing meanscomprises an equalizer (114), and the ratio between the output amplitudeof the equalizer at the frequency of the longest mark and the outputamplitude of the equalizer at the frequency of the shortest mark is 3 dBor less, provided that the longest mark and the shortest mark are fromthe same classification.

Further preferably according to a twenty-eighth aspect of the presentinvention, the pattern signal contains an adjustment signal forobtaining a DSV of 0.

A twenty-ninth aspect of the present invention relates to a recordingand reproducing apparatus for recording and reproducing a data recordingmedium having a plurality of tracks, marks formed by emitting to a trackin the data recording medium an optical beam modulated by one or aplurality of drive pulses where a number of the drive pulses isdetermined according to a length of a mark part in the original signalto be recorded to the track, and a control information recording areafor recording information using the marks and spaces between the marks,and having recorded thereto at least a first pulse position Tu value anda last pulse position Td value whereby at least a first pulse positionTu and a last pulse position Td of the drive pulse is changed so as tomake a reproduction jitter a specific value or less. This recording andreproducing apparatus comprises: means (1505-1508, 1512-1517) forreproducing a first pulse position Tu and a last pulse position Tdprerecorded to the data recording medium; means (1520) for storing thereproduced first pulse position Tu and last pulse position Td; means(1510) for generating a drive pulse based on a data recording signal,and correcting the generated drive pulse based on the first pulseposition Tu and last pulse position Td; means (109, 103-106) foremitting an optical beam based on the corrected drive pulses to formspaces and marks on the data recording medium.

Further preferably according to a thirtieth aspect of the presentinvention, the reproducing means comprises an equalizer (1514), and theratio between the output amplitude of the equalizer at the frequency ofthe longest mark and the output amplitude of the equalizer at thefrequency of the shortest mark is 3 dB or less.

A thirty-first aspect of the present invention relates to amanufacturing apparatus for manufacturing a data recording medium havinga plurality of tracks, marks formed by emitting to a track in the datarecording medium an optical beam modulated by one or a plurality ofdrive pulses where a number of the drive pulses is determined accordingto a length of a mark part in the original signal to be recorded to thetrack, and a control information recording area for recordinginformation using the marks and spaces between the marks, and havingrecorded thereto at least one of a first pulse position Tu value and alast pulse position Td value whereby at least one of a first pulseposition Tu and a last pulse position Td of the drive pulse is changedso as to make a reproduction jitter a specific value or less. Thisapparatus comprises: means (2701) for storing previously obtained firstpulse position Tu and last pulse position Td values for a drive pulsesequence; adjustment method information storage (2702) for storinginformation indicative of a pulse position adjustment method; means(2703) for converting the adjustment method information, first drivepulse position Tu, and last drive pulse position Td to a signal forrecording, and generating a recording signal; and laser generating means(2704, 2705, 2706) for generating a laser beam based on the recordingsignal.

Other objects and attainments together with a fuller understanding ofthe invention will become apparent and appreciated by referring to thefollowing description and claims taken in conjunction with theaccompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram of an optical data recording device accordingto a first embodiment of the present invention;

FIG. 2 illustrates signals used in the first embodiment shown in FIG. 1;

FIG. 3 illustrates recording pulse sequences in the first embodimentshown in FIG. 1;

FIG. 4 shows exemplary pulse movement tables in the first embodimentshown in FIG. 1;

FIG. 5 is used to describe a grouping method in the first embodimentshown in FIG. 1;

FIG. 6 is used to describe a grouping method in the first embodimentshown in FIG. 1;

FIG. 7 is used to describe a grouping method in the first embodimentshown in FIG. 1;

FIG. 8 is used to describe a grouping method in the first embodimentshown in FIG. 1;

FIG. 9 is used to describe a grouping method in the first embodimentshown in FIG. 1;

FIG. 10 is a frequency characteristic diagram for a reproductionequalizer in the first embodiment shown in FIG. 1;

FIG. 11 illustrates signals used in the first embodiment shown in FIG.1;

FIG. 12 illustrates signals used in the first embodiment shown in FIG.1;

FIG. 13 illustrates signals used in the first embodiment shown in FIG.1;

FIG. 14 illustrates signals used in the first embodiment shown in FIG.1;

FIG. 15 is a block diagram of an optical data recording device accordingto a second embodiment of the present invention;

FIG. 16 is a plan view of a data recording medium in the secondembodiment shown in FIG. 15;

FIG. 17 illustrates signals used in the second embodiment shown in FIG.15;

FIG. 18 illustrates recording pulse sequences in the second embodimentshown in FIG. 15;

FIG. 19 shows exemplary pulse movement tables in the second embodimentshown in FIG. 15;

FIG. 20 is a waveform diagram for describing first pulse movementaccording to the present invention;

FIG. 21 is a waveform diagram for describing last pulse movementaccording to the present invention;

FIG. 22 is a waveform diagram for describing first pulse widthadjustment according to the present invention;

FIG. 23 is a waveform diagram for describing last pulse width adjustmentaccording to the present invention;

FIG. 24 shows alternative pulse movement tables according to the presentinvention;

FIG. 25 is a plan view of a data recording medium according to thepresent invention;

FIG. 26 is a plan view of a further data recording medium according tothe present invention;

FIG. 27 is a block diagram of a system for cutting an optical diskmaster according to the present invention; and

FIG. 28 illustrates signals used in the first embodiment shown in FIG.1.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The preferred embodiments of the present invention are described belowwith reference to the accompanying figures.

An optical data recording method according to a preferred embodiment ofthe present invention is described next below with reference to theaccompanying figures. FIG. 1 is a block diagram of an optical datarecorder according to a first preferred embodiment of the presentinvention. It is to be noted that this optical data recorder is usedprimarily by manufacturers and other commercial users for manufacturingoptical disks.

Shown in FIG. 1 are: an optical disk 101 having a plurality ofconcentric or spiral tracks, spindle motor 102, semiconductor laser 103,collimator lens 104, beam splitter 105, objective lens 106, collectivelens 107, photodetector 108, laser drive circuit 109, pulse movingcircuit 110, delay circuits 128 and 129 each having the same delay time,pulse generator 111, preamp 112, low pass filter 113, reproductionequalizer 114, digitizing circuit 115, PLL 116, demodulation and errorcorrection circuit 117, reproduction data signal 118, power settingcircuit 119, pulse position offset measuring circuit 120, switch 121,switch contacts 122, 123, and 124, pattern signal generator 125, bus 126connecting pulse position offset measuring circuit 120 and pulse movingcircuit 110, and memory 127 for storing a table recording pulse movementinformation.

Memory 127 stores the two tables shown in FIG. 4(b). These two tablesare modified by the method of the present invention, and are thenrewritten as the two tables shown in FIG. 4(a).

The optical data recorder shown in FIG. 1 is for generating a table suchas shown in FIG. 4(a). The table shown in FIG. 4(a) and generated by therecorder shown in FIG. 1 is then transferred to a memory in anotherrecording device such as shown in FIG. 27, and is recorded to apredetermined recording area on all manufactured optical disks.

It is to be noted that the optical head of the optical data recordershown in FIG. 1 comprises the semiconductor laser 103, collimator lens104, beam splitter 105, objective lens 106, collective lens 107, andphotodetector 108. When an optical disk 101 is loaded to the opticaldata recorder, the optical head moves to an area used for determiningthe optimum positions for the start position and end position of eachmark.

This area for determining the optimum start and end positions is an areaat the inside circumference area or outside circumference area of thedisk, and is outside of the user data recording area. An exemplary areais the drive test zone of the disk. Switch 121 switches contact 122 tocontact 123 at this time.

It is to be noted that if limited specifically to recording devices usedby a manufacturer of optical disks, this area for determining theoptimum start and end positions can be the user data area.

The power setting circuit 119 sets the laser drive circuit 109 to eitherpeak power or bias power. At this time the output signal from patternsignal generator 125 is passed by switch 121 to the pulse generator 111.Signal flow from the pulse generator 111 is described further below withreference to FIG. 2.

Shown in FIG. 2 are a first pattern signal 201, which is the outputsignal from the pattern signal generator 125; output signal 202 from thepulse generator 111; output signal 203 from the pulse moving circuit110; and mark pattern 204 formed in the recording track of the opticaldisk 101 as a result of modulating laser power output between peak powerand bias power levels according to output signal 203. It is to be notedthat while signals 201, 202, and 203 are not generated on the same timebase, for convenience they are shown with corresponding parts in eachsignal aligned vertically.

In first pattern signal 201, mark parts 209, 211, 213, 215, 217, and 219are the parts of the signal whereby a mark is to be formed on the disk,and space parts 210, 212, 214, 216, 218, and 220 are the parts of thesignal that appear as a space on disk. It is further assumed below thatmark part 209 follows space part 220 such that first pattern signal 201comprises a repeating pattern of parts 209 to 220.

For example, when data generated by (2,10) run-length limited modulationis recorded using a mark edge recording method, the marks and spaceshave a shortest length of 3T and a longest length of 11T where T is thereference period. Mark part 209 is a 6T signal (a 6T mark part below),space part 210 is a 6T space, 211 is a 3T mark, 212 is a 6T space, 213is a 6T mark, 214 is a 6T space, 215 is a 6T mark, 216 is a 4T space,217 is a 6T mark, 218 is a 6T space, 219 is a 7T mark, and 220 is a 6Tspace.

Note that if DSV is the difference of the sum of mark and space lengthsin a specific period, a reproduction signal with a small dc component orlow frequency component can be obtained when the marks and spaces arereproduced by inserting signals 219 and 220 whereby a DSV ofsubstantially zero can be obtained. Reproducing a signal with many dccomponents or low frequency components can result in the digitizingcircuit 115 erroneously generating a signal with the wrong sequence of0s and 1s.

To prevent this, a 7T mark part 219 and 6T space part 220 are insertedto the first pattern signal 201 as a compensation signal assuring thatthe DSV is substantially 0. More specifically, first pattern signal 201is generated so that the sum (34T) of the periods of mark parts 209,211, 213, 215, 217, and 219 is equal to the sum (34T) of the space parts210, 212, 214, 216, 218, and 220. DSV is calculated by adding theperiods of the mark parts as positive values and the periods of thespace parts as negative values. As a result, the DSV of first patternsignal 201 is 0.

This first pattern signal 201 is converted to a pulse sequence by thepulse generator 111, resulting in pulse generator output signal 202.Pulse output from the pulse generator 111 corresponding to marks oflengths from 3T to 11T is shown in FIG. 3.

Referring by way of example to a 6T signal in FIG. 3, the pulse at thestart of the signal is referred to as the first pulse 301, and the pulseat the end of the signal is the last pulse 304. The pulses between thefirst pulse 301 and last pulse 304 are referred to as multiple pulses302 and have a constant period.

In a 6T mark there are two multiple pulses 302, in a 7T mark there arethree, and in a 5T mark there is one. It will thus be obvious that thenumber of multiple pulses 302 between the first and last pulsesincreases by one with each 1T increase in signal length, and decreasesone with each 1T decrease in signal length. A 4T mark, thereforecomprises only the first and last pulses, and has no multiple pulses 302therebetween. In addition, a 3T mark comprises just one pulse.

It is to be noted that in this preferred embodiment the time-base lengthof the first pulse is 1.5T, the last pulse is 0.5T, and the length ofthe multiple pulses is also 0.5T. The invention shall not be so limited,however, and the length, count, or period of these pulses can be variedas necessary according to the structure of the optical disk 101.

As noted above, first pattern signal 201 and pulse generator outputsignal 202 are not on the same time base. However, the differencebetween the leading edge of first pattern signal 201 and the leadingedge of the first pulse of the pulse generator output signal 202 is thesame for any particular mark parts, and the difference between thetrailing edge of the first pattern signal 201 and the trailing edge ofthe last pulse of pulse generator output signal 202 is also the same forany particular mark parts.

The pulse generator output signal 202 is input to the pulse movingcircuit 110, which generates and outputs a signal 203 in which thepositions of the first pulse and last pulse are moved. FIG. 4 shows thecombinations of marks and spaces used for shifting the first pulse andlast pulse positions.

FIG. 4(a) shows the pulse movement tables after correction by the methodof this present invention, and FIG. 4(b) shows the tables beforecorrection. Symbols 3S3M, 4S3M, and so forth in the tables in FIG. 4(a)are a type of address, and are indicative of the signal type as well asthe value written to that address. When read as an address, the value3S3M, for example, represents a signal in which a 3T mark follows a 3Tspace. As will be described more fully below, the value of the firstpulse movement TF stored at the place indicated by 3S3M is the movementrequired when a 3T mark follows a 3T space.

These first pulse movement TF values are obtained by, for example, atrial and error process using a particular optical test disk, and theresulting values are compiled in the tables in FIG. 4(a). The content ofthe completed table is stored for all optical disks having the samestructure as the optical test disk. Predetermined initial values arestored in the table on the left in FIG. 4(b) for the first pulse. Thetable on the right in FIG. 4(b) stores the initial values beforecorrecting the last pulse movement.

The position of the first pulse changes according to the length of themark and the immediately preceding space. In this preferred embodiment,the marks and spaces are separated into three groups, that is, 3T, 4T,and 5T or longer. A total of nine different last pulse positions aretherefore defined.

FIG. 20 is an enlarged view of the 6T mark 217 in the first patternsignal 201 shown in FIG. 2, and the corresponding part in the pulsegenerator output signal 202. As shown in the figure, a 4T space 212 isimmediately before the 6T mark 217. A 4T space followed by a 6T markbelongs to the 4S5M group in the left table in FIG. 4(a). Correcting theinitial first pulse movement TF stored for this group is describedbelow.

The pattern signal generator 125 in the optical data recorder shown inFIG. 1 generates a first pattern signal 201. This first pattern signal201 is sent to the pulse generator 111, delay circuit 129, pulseposition offset measuring circuit 120, and memory 127. As noted above,the two tables shown in FIG. 4(b) are prestored to memory 127. The pulseposition offset measuring circuit 120 also stores the first patternsignal 201, which is used for comparison with the reproduction signalduring data reproduction. The pulse generator 111 generates the outputsignal 202 required for recording the pattern signal. Referring to thesignals shown on the top two rows in FIG. 3, for example, the pulsegenerator 111 generates a first pulse 301 corresponding to the risingedge of the mark in the first pattern signal 201, then outputs multiplepulses 302, and last pulse 304.

The pulse generator output signal 202 is delayed a predetermined periodby the delay circuit 128, and then passed to the pulse moving circuit110. This predetermined delay period is 13T in this exemplaryembodiment. The first pattern signal 201 is analyzed in memory 127 todetermine to which of the 18 signal groups, that is, 3S3M, 3S4M, 3S5M,4S3M, 4S4M, 4S5M, 5S3M, 5S4M, 5S5M, 3M3S, 4M3S, 5M3S, 3M4S, 4M4S, 5M4S,3M5S, 4M5S, and 5M5S, the signal in the preceding 10T or longer periodbelongs. For example, if a 4T space 216 is followed by a 6T mark 217 inthe first pattern signal 201 from the pattern signal generator 125,memory 127 detects that the signal belongs to the 4S5M group. Inresponse to this determination, memory 127 then reads and outputs to thepulse moving circuit 110 the amount of movement stored in the table at4S5M0. The initial 4S5M0 movement value is read from the table the firsttime a movement value is read. The pulse moving circuit 110 then movesthe first pulse of the pulse generator output signal 202 suppliedthereto after a predetermined delay based on the initial movement valueread from 4S5M0.

Movement of the first pulse is described in further detail below withreference to FIG. 1 and FIG. 20. When the pulse moving circuit 110 isnotified by memory 127 that a pattern belonging to a specific group willsoon arrive from the delay circuit 129, it also receives the first pulsemovement TF for that pattern from the memory 127. For example, when thememory 127 informs the pulse moving circuit 110 that a pattern belongingto the 4S5M group, that is, a 4T space 216 following by a 6T mark 217,will arrive from the delay circuit 129, it also sends the first pulsemovement TF read for the 4S5M0 group. The pulse moving circuit 110 thenbegins counting first pulse movement TF at the rising pulse edge of the6T mark 217 received from the delay circuit 129, that is, at time R1 inFIG. 20. Output of the first pulse from the delay circuit 128 is delayedfor the period counted by the pulse moving circuit 110, that is, forpulse movement TF1.

When pulse movement is referenced to the rising edge R1 of the firstpattern signal 201, for example, first pulse movement TF1 is expressedas the time difference from reference time R1 as shown in FIG. 20. Inthis exemplary embodiment, pulse movement TF is approximately 3 ns. Itis to be noted that the first pulse is moved without changing the pulsewidth.

The pattern signal shown in FIG. 2 contains signal components belongingto four of the 18 groups in the table shown in FIG. 4(a): type 3M5S inperiod 221, type 5S3M in period 222, type 4S5M in period 223, and type5M4S in period 224. Each of the pulse signal components corresponding tothese four types in first pattern signal 201 are therefore moved.

The laser is therefore driven according to these moved pulses to recordthe actual marks. The resulting marks 204 are shown in FIG. 2. In apreferred embodiment of the present invention, the first pattern signal201 comprising elements 209 to 220 as shown in FIG. 2 is outputrepeatedly and recorded around one track. When the recording to onecomplete track is thus completed, the track is reproduced. As will bedescribed more fully below, reproduction includes converting an opticalsignal from the photodetector 108 to an electrical signal, and thenprocessing this electrical signal with preamp 112, low pass filter 113,reproduction equalizer 114, and digitizing circuit 115 to obtainreproduction signal 205. The reproduction signal 205 is input to thepulse position offset measuring circuit 120. The reproduction signal 205from a single track is thus input repeatedly to the pulse positionoffset measuring circuit 120. The pulse position offset measuringcircuit 120 thus reads each of the periods 221, 222, 223, and 224associated with different signal types multiple times, and calculatesthe average for each period.

The pulse position offset measuring circuit 120 compares the periods221, 222, 223, 224 corresponding to the types obtained in the recordedfirst pattern signal 201 during recording, and the averages for the sameperiods obtained from the reproduction signal 205 to detect whether anyshifting in pulse position has occurred. Using, by way of example, thesignals recorded and reproduced as described above, the combined time ofthe 4T space 216 and 6T mark 217 in the first pattern signal 201 iscompared with the average obtained for the corresponding period 224 inthe reproduction signal 205, and the difference therebetween isobtained. If there is a difference, the pulse position offset measuringcircuit 120 determines that the pulse position shifted, and thecalculated difference is therefore sent to memory 127. Because thisdifference is the result of the initial movement value 4S5M0, thisinitial movement value 4S5M0 is increased or decreased in memory 127according to the difference, thereby correcting the stored movementvalue. This corrected value is then overwritten to type 4S5M.

It is to be noted that the stored movement value is corrected andoverwritten to 4S5M using a single feedback loop (through 110, 109, 108,112, 115, 120, 126) in the above exemplary embodiment. It will beobvious, however, that a plurality of feedback loops can bealternatively used to correct the value of the first pulse movement TFas shown in FIG. 20.

Movement of the last pulse position is similarly corrected. That is, thelast pulse position movement changes according to the mark length andthe length of the following space. In this exemplary embodiment marksand spaces are separated into three groups based on length, 3T, 4T, and5T or longer, and pulse position movement is defined for each of thenine possible mark/space combinations. The last pulse movement TL isthen calculated using the same method used to calculate the first pulsemovement TF.

FIG. 21 is an enlarged view of the part of the pulse generator outputsignal 202 corresponding to the 6T mark 215 in the first pattern signal201 shown in FIG. 2. The last pulse movement TL is corrected in the samemanner as the first pulse movement TF described above. In the case ofthe last pulse movement TL, however, the period from time reference R2offset 2T forward of the trailing edge of the mark to the trailing edgeof the last pulse is called the time interval, and this time interval iscorrected by means of the loop described above with reference to thefirst pulse. The last pulse movement TL is approximately 13 ns in thisexemplary embodiment. It is to be also noted that the width of the lastpulse does not change even though the amount of last pulse movement TLchanges, and in this exemplary embodiment the pulse width remains thesame with the pulse simply shifted on the time axis.

The output signal 206 from the pulse moving circuit 110 obtained usingthe corrected pulse movement tables shown in FIG. 4(a), the marks 207recorded as a result of this output signal 206, and the reproductionsignal 208 reproduced from these marks 207, are also shown in FIG. 2.While the reproduction signal 205 obtained using the original,uncorrected pulse movement table (FIG. 4(b)) is not identical to theoriginal pattern signal 201, there is substantially no differencebetween the reproduction signal 208 obtained using the corrected pulsemovement table (FIG. 4(a)) and the original pattern signal 201.

It is to be noted that four of the eighteen pulse movement values arecorrected as described above using the first pattern signal 201 shown inFIG. 2. The other values are similarly corrected using other patternsignals. More specifically, types 4M5S, 5S4M, 3S5M, and 5M3S arecorrected using a pattern signal 1101 as shown in FIG. 11; types 4M4S,3M3S, 4S4M, 3S3M are corrected using a pattern signal 1201 as shown inFIG. 12; types 4M3S, 4S3M are corrected using a pattern signal 1301 asshown in FIG. 13; types 3M4S, 3S4M are corrected using a pattern signal1401 as shown in FIG. 14.

It is to be noted that types 5M5S and 5S5M can be corrected using apattern signal 2801 as shown in FIG. 28, or a default value therefor canbe simply defined. It is to be noted that types 5M5S and 5S5M arepreferably corrected before the other types. This is because these marksand spaces have the longest period and are therefore least affected bythermal interference. The delay period is therefore small, and can beused as a reference value for determining the other delay periods.

The signal types used for changing the movement of the first pulse andlast pulse are determined based on the three major factors describedbelow.

The first factor is the effect of heat accumulation in the recordingfilm when marks are recorded, the amount of thermal interference, andthe difference in the amount of thermal interference resulting from thespecific mark-space combination. Note that, as described above, thermalinterference refers to the process whereby heat at the end of a recordedmark transfers through the following space and affects the heatingprocess at the beginning of the next mark, and heat at the beginning ofa next recorded mark conversely travels back through the preceding spaceand affects the cooling process at the end of the preceding mark.

The affects of heat accumulation in the recording film can be reduced byinserting a plurality of multiple pulses between the first and lastpulses, and emitting a laser beam of the lowest power level required formark formation. These heat accumulation effects cannot be completelyeliminated, however, because the multiple pulses are formed with aconstant period in order to simplify the pulse generator 111.

The extent of the effect of heat accumulation and thermal interferenceis also dependent upon numerous factors, including the structure of theoptical disk 101, properties of the recording film, recording pulse, thelinear speed used for recording to optical disk 101, and the length ofthe shortest mark. The effect of heat accumulation and thermalinterference can also be attenuated to a certain degree by optimizingeach of these influencing factors. To more fully understand this, let usfocus on how the effects of heat accumulation and thermal interferencevary with different combinations of marks and spaces.

As will be known from FIG. 4(a), each first pulse is classified as oneof nine types or groups, which are used for determining the movement ofthe first and last pulses. A method for determining which of these ninetypes to use based on the above-noted first factor is described nextwith reference to FIG. 5 to FIG. 9. FIG. 5 shows a method fordetermining the dependency of the elongation of the starting position ofan 11T mark on the space preceding the 11T mark.

Shown in FIG. 5 are the original signal 500, that is, the two-valuewaveform of the signal used for recording, marks 501 recorded to thedata recording medium, and reproduction signal 502, that is, thetwo-value waveform of the signal reproduced from the marks 501 recordedto the disk. Original signal 500, marks 501, and reproduction signal 502are the result of recording marks with a space (S×T) sufficiently longfor an 11T mark recorded between the marks. Intersymbol interference isthus minimized as a result of this sufficiently long space.

It is to be noted that space tsl in the original signal 500 is ideallyequal to the time interval of space tm11 in the reproduction signal 502.The positions of the first and last pulses are moved to more closelyapproach this ideal. If the position of the mark start position only isconsidered when determining how much to move the marks, the first andlast pulses can be categorized into approximately three groups. A methodfor determining the mark start position group is described more fullybelow with reference to original signal 520, marks 521, and reproductionsignal 522 describe below.

The original signal 520 is the two-value waveform used for recording. Inthis case, however, the space ts21 between the two 11T marks is shorterthan that shown in the above described original signal 500. As a result,heat at the trailing end of 11T mark 524 transfers through space 525 tothe next 11T mark 526, thus accelerating the start of 11T mark 526. Thenominal length of 11T mark 526 is thus increased by length a2.

As a result, the time interval of space ts31 in reproduction signal 522corresponding to space ts21 in the original signal 520 is shortened, andthe correct reproduction signal cannot be obtained. A correctreproduction signal can be obtained, however, by predicting theelongation at the start of 11T mark 526, and delaying the rising edge ofthe mark part tm22 in the original signal 520. The specific delaydepends on the length of the space ts21. The length of the space ts21 istherefore varied for each time T from 3T to 11T, an 11T mark is recordedfor each space ts21, and edge distance 527 is measured for each case.

The results of these measurements are graphed in FIG. 6. The horizontalaxis shows the length 3T to 11T of each space ts21 in original signal520, and the vertical axis shows the difference of the combined lengthof mark part tm20 and space part ts21 in the original signal 520 minusthe edge distance r 527. As the space length decreases, the point atwhich 11T mark 526 starts moves forward, that is, closer to thepreceding pulse, due to thermal interference when the space is short,such as 3T or 4T.

FIG. 7 shows one way of combining spaces of substantially the samelength into common groups based on the values shown on the vertical axisin FIG. 6. Spaces of substantially different length are placed inseparate groups. This method produces three groups: 3T spaces, 4Tspaces, and spaces of 5T or longer.

These results and groups are further mapped in FIG. 8. Shaded cellsindicate space/mark combinations for which measurements have beenobtained. Bold lines indicate the groups.

As described with reference to FIG. 5, elongation at the start of an 11Tmark varies according to the length of the immediately preceding space,and can be separated into the above three groups, 3T, 4T, and 5T orlonger.

FIG. 9 shows the results of the evaluation described above withreference to FIG. 5 to FIG. 8 performed for all rows and columns. Itwill be known from FIG. 9 that both marks and spaces are preferablyseparated into the above three or more groups, 3T, 4T, and 5T or longer,for determining first pulse movement.

Last pulse movement varies according to the mark length and immediatelyfollowing space. For the same reasons that apply to the first pulse,last pulse movement is preferably determined based on the same three ormore groupings, that is, 3T, 4T, and 5T or longer, of marks and spacesdescribed above.

It is to be noted that when measurement results are substantially equal,such as from 5T to 11T, in adjacent cells in the maps shown in FIG. 9,those cells are grouped together. This makes it possible to reduce thescale of the pulse moving circuit 110.

As will be known from the above description, by focusing on thedifference in size resulting from specific mark/space combinations, andplacing combinations where the space length is 3T or 4T into a groupseparate from combinations where the space length is 5T or longer, thispreferred embodiment of the invention can control first pulse movementand last pulse movement according to the mark/space pattern, and canthereby achieve recording with little jitter.

In addition, by focusing on the difference in size resulting fromspecific mark/space combinations, and placing combinations having aspace length of 3T and combinations having a space length of 4T intoseparate groups, this preferred embodiment of the invention can controlfirst pulse movement and last pulse movement according to the mark/spacepattern.

The properties of the reproduction equalizer 114 are a second factor.Reproduction equalizer 114 properties depend on such factors as the beamspot size and shortest mark length. The beam spot size is determined bythe wavelength of the semiconductor laser 103 and the aperture of theobjective lens 106.

A method of grouping marks and spaces in order to change first pulsemovement and last pulse movement due to this second factor is describednext below with reference to FIG. 10.

FIG. 10 is a typical graph of the frequency characteristic of thereproduction equalizer 114. This shows the amplitude ratio of theequalizer output signal to the input signal, signal frequency is shownon the horizontal axis, and output amplitude is shown on a logarithmicscale on the vertical axis. The frequency of 3T, 4T, 5T, and 11T signalsis shown along the horizontal axis. Note that the frequency of a 3Tsignal is high, the marks recorded and reproduced for a 3T signal aretherefore small, and the amplitude of the reproduced optical signal istherefore low. Equalizer characteristics are therefore set to increasethe output amplitude to compensate for this attenuation of the opticalfrequency characteristic. This can be accomplished by using a high passfilter or a bandpass filter with a peak at a frequency slightly higherthan 3T, with or without an amplifier used in combination.

The slope of the curve, that is, the difference in the output amplitudeof a high frequency signal in which mark or space length is 3T, and theoutput amplitude of a low frequency signal in which mark or space lengthis 11T, increases as the shortest mark length decreases. As a result,the difference between, for example, the output amplitude at a frequencyof 5T and the output amplitude at a frequency of 11T, also increases.

If marks for which the difference in output amplitude is great areincluded in the same group when separating the marks for changing firstand last pulse movement, reproduction equalizer 114 properties preventcorrect edge position reproduction even if the first and last pulses arerecorded to specifically eliminate the effects of heat accumulation inthe recording film and thermal interference.

It is therefore preferable for the difference in the output amplitudecharacteristic of the reproduction equalizer 114 to be as small aspossible for all marks in the same group.

It is further preferable for the ratio between the output amplitude ofthe reproduction equalizer 114 at the frequency of the longest mark tothe output amplitude of the reproduction equalizer 114 at the frequencyof the shortest mark in the plurality of marks in the same group to be 3dB or less. This value, 3 dB or the square root of 2, is relativelycommonly used when working with frequency characteristics.

In other words, regardless of frequency, when signals of the sameamplitude are input, the amplitude ratio of the input signal and outputsignal from the equalizer will always be a difference equal to thesquare root of 2. By controlling the output amplitude ratio to 3 dB orless as a threshold value for grouping signals together as in thispreferred embodiment of the invention, distortion error introduced bythe equalizer during reproduction is reduced, and recording andreproducing with less jitter can be achieved.

It is to be noted that in mark edge recording using a semiconductorlaser 103 with a 650 nm wavelength, an objective lens 106 with anaperture of 0.6, a shortest mark length of 0.595 μm, and (2,10)run-length limited modulation, marks shorter than 5T, that is, 3T and 4Tmarks, are preferably not included in the same group as 11T marks.Further considering the size of the pulse moving circuit 110, 5T andlonger marks, or 6T and longer marks, are preferably included in thesame group. In this exemplary embodiment, T is approximately 30 ns, 3Tis approximately 90 ns, and 11T is approximately 330 ns.

A third factor is the scale of the pulse moving circuit 110 and thedesired precision with which pulse movement is determined, and thelimited scale of the pattern signal generator 125 and memory 127.

Based on the above described first and second factors, marks or spaceswith a great difference in heat accumulation or thermal interference areplaced into different groups, and marks resulting in a significantlydifferent output amplitude from the reproduction equalizer are alsoplaced in different groups. However, the number of storage registersincreases as the number of groups increases, and this increases thescale of the pulse moving circuit 110. In addition, if the number ofregisters is increased, the number of patterns used for determining thevalues stored to the registers also increases, and the scale of thepattern signal generator 125 therefore also increases. Yet further, thetime required to set the registers increases whether the register valuesare set at the factory or by the end user, and the recording track spacerequired for setting the registers also increases.

It is therefore desirable to minimize the number of groups used fordetermining first and last pulse movement.

By grouping marks of 5T and longer in the same group as describedaccording to this preferred embodiment, the scale of the pulse movingcircuit 110, and the scale of the pattern signal generator 125, can bothbe minimized.

Although determining the optimum grouping of marks and spaces isaffected by several factors, the three factors described above areconsidered in particular to determine the group types shown in FIG. 4 inthe present embodiment.

It is to be noted that a predetermined initial value is set as shown inFIG. 4(b) before pattern signal recording. These initial values can beseparately determined from experience, or they can be all set to thesame value. If the same initial value is used for all, the value, forexample, 1 ns, stored for the first pulse movement in a 5S5M pattern inthe left table in FIG. 4(b), for example, is preferably stored for allpatterns. In the case of the right table in FIG. 4(b), the value storedfor 5M5S is used. Note, further, that in this case the value set for the5S5M pattern is determined so that the time between first pulse 301 andmultiple pulses 302 is 0.5T as shown in FIG. 3, and the value set for5M5S is determined so that the time between multiple pulses 302 and lastpulse 304 is 0.5T.

It will also be obvious that the values set for 5S5M and 5M5S can alsobe determined using other methods. An example is shown in FIG. 28.

As shown in FIG. 28, the pattern signal 2801 of the pattern signalgenerator 125 in this example has a single period of 6T. Also shown areoutput signal 2802 from the pulse generator 111, output signal 2803 fromthe pulse moving circuit 110, and marks 2804 formed in the recordingtrack of the optical disk 101 as a result of modulating laser poweroutput between peak power and bias power levels according to outputsignal 2803. It is to be noted that while signals 2801, 2802, and 2803are not generated on the same time base, for convenience they are shownwith corresponding parts in each signal aligned vertically.

The pattern signal 2801 in this case represents marks and spaces with asimply repeating 6T period, and thus contains types 5S5M and 5M5S of theeighteen pattern types shown in FIG. 4(a). The laser is then drivenbased on drive signal 2803 in FIG. 28 to record the marks 2804. In thisexemplary embodiment, pattern signal 2801 in FIG. 28 is repeatedlyrecorded around one complete circumference of the recording track. Whenthis track is recorded, it is then reproduced. Reproduction includesconverting an optical signal from the photodetector 108 to an electricalsignal, and then processing this electrical signal with preamp 112, lowpass filter 113, and reproduction equalizer 114. The reproduction signal2805 from the reproduction equalizer 114 is applied to an asymmetrymeasuring circuit 130 and a digitizing circuit 115. The digitizingcircuit 115 adjusts the slice level signal 2809 so that the output levelcorresponding to a mark and the output level corresponding to a space inthe output signal of the digitizing circuit are at equal intervals, andapplies this slice level signal 2809 to the asymmetry measuring circuit130.

The asymmetry measuring circuit 130 compares the average of the high2811 and low 2810 peak values of the reproduction signal 2805 with theslice level signal 2809. When the difference therebetween is apredefined level or greater, the lengths of the marks 2804 and spacesare not equal. This difference is attributable to a shift in the firstpulse and last pulse positions. Initial movement values 5S5M0 and 5M5S0are therefore corrected according to the sign of the difference so that,for example, the first pulse and last pulse each move the same time-basedistance in opposite directions. The corrected values are thenoverwritten to memory 127.

It is to be noted that the stored movement values are corrected andoverwritten to 5M5S and 5S5M using a single feedback loop (through 110,109, 108, 112, 115, 120, 126) in the above exemplary embodiment. It willbe obvious, however, that a plurality of feedback loops can bealternatively used. As a result, 5S5M and 5M5S values whereby 6T markscan be recorded at the correct length can be obtained. By thuscorrecting the physical length of a mark used as a reference, marks inother groups can also be recorded at the correct length, and recordingwith less jitter can be achieved.

The output signal 203 from the pulse moving circuit 110 is input to thelaser drive circuit 109 whereby laser power is modulated so that thelaser emits at peak power while the output signal 203 is high, and emitsat bias power while the signal is low, to form a mark sequence 204 asshown in FIG. 2.

During reproduction, the collimator lens 104 converts the laser beamemitted from the semiconductor laser 103 to parallel light, which isthen incident on the beam splitter 105. Light passing the beam splitter105 is focused to a light spot by the objective lens 106, and emitted tothe optical disk 101.

Light reflected from the optical disk 101 is then collected by theobjective lens 106, and passed back to the beam splitter 105. Lightreflected by the beam splitter 105 is collected by collective lens 107,and focused on photodetector 108.

The photodetector 108 converts light incident thereon to an electricalsignal, which is then amplified by the preamp 112. The output signalfrom the preamp 112 is then passed through the low pass filter 113whereby high frequency signal components are blocked. The reproductionequalizer 114 then equalizes the signal, which is next binarized by thedigitizing circuit 115 using a predetermined slice level. A reproductionsignal 205 converted to a sequence of 0s and 1s is thus output from thedigitizing circuit 115 to the pulse position offset measuring circuit120. The pulse position offset measuring circuit 120 measures thespecific edge intervals 221, 222, 223, and 224 in the reproductionsignal 205.

If the measured edge interval 221 in FIG. 2 is longer than the normal 9Tinterval, the setting for last pulse movement 3M5S in FIG. 4(a) isreduced by the difference between the measured interval 221 and thenormal 9T interval from the current setting of 3M5S0 by way of bus 126.The setting for first pulse movement 5S3M in FIG. 4(a) is similarlyincreased from the current 5S5M0 setting by the difference between theedge interval 222 and the normal 9T interval by way of bus 126 if theedge interval 222 is longer than the normal 9T interval. The valuesstored for 4S5M and 5M4S are likewise corrected based on the measurededge intervals 223 and 224.

When these four settings are updated, the first pattern signal 201 isagain recorded and the edge intervals are measured. This process isrepeated until the difference between the normal interval and themeasured edge interval is below a predetermined threshold levelsimultaneously for all four edge intervals. Note that when measuring theedge intervals, the edge that is not moved is the falling edge of 6Tmark 209, and the immediately following space is 6T space 210, in thecase of edge interval 221, for example. In the case of edge interval222, the rising edge of 6T mark 213 is not moved, and the immediatelypreceding space is 6T space 212.

The mark and space between which are located the edge that is not movedwithin a mark/space pattern are referred to herein as a referencesignal. This edge is further referred to as the reference edge. If thereference edge moves in conjunction with an edge that is moved, movementsettings cannot be correctly determined because there is no fixed pointof reference. The position of the reference edge must therefore mustremain stationary and cannot move in conjunction with the edge that ismoved.

Furthermore, even when the edge in the reference signal does not changein conjunction with an edge that is moved, it may be necessary to changethe reference signal so that the reference edge does not move inconjunction with the shifted edge. For example, if the reference signalincludes a mark of the shortest possible length, it is necessary tochange the reference signal so that the reference signal edge does notchange at any of the movement settings defined for the shortest marks.Considering the potential for setting variations, the reference marksare preferably fixed.

If the reference signal is included in the same group as the longestsignal, the same reference signal can be used for all settings shown inFIG. 4(a), and mark start and end positions can be more accuratelydetermined in various mark/space combinations.

Though small, there are also differences in the change of the mark edgeposition even in the longest signal group because of differences in heataccumulation and thermal interference within the group for changingfirst pulse and last pulse movement. However, by selecting as thereference signal a mark/space signal with a high frequency of occurrencethat also belongs to the group containing the longest possible signal asin this preferred embodiment of the invention, an overall reduction inthe occurrence of imprecise edge positions can be achieved.

Furthermore, though small there are also differences in the outputamplitude of the reproduction equalizer when reproducing differentmark/space signals in the group containing the longest possible markbecause of differences in the output amplitude of the reproductionequalizer 114 within the group for changing first pulse and last pulsemovement. However, by selecting as the reference signal a mark/spacesignal with a high frequency of occurrence that also belongs to thegroup containing the longest possible signal as in this preferredembodiment of the invention, the occurrence of imprecise edge positionscan be reduced in the overall recording and reproducing system.

By thus achieving an overall reduction in the occurrence of edges atimprecise positions, the probability of reliable error correction by thedemodulation and error correction circuit 117 during actual datarecording is improved.

It is to be noted that the frequency of signal occurrence increases andthe output amplitude of the reproduction equalizer increases as signallength decreases. Selecting the reference mark therefore involves atrade-off between the frequency of occurrence and the output amplitude.Furthermore, while marks and spaces of 5T or longer are in the samesignal group in this preferred embodiment of the invention, a 6Treference mark is used in consideration of the reproduction equalizercharacteristics.

It is to be further noted that the initial values set for 3S3M0 and3M3S0 are selected so that the reference marks will be recorded with thecorrect length. Different initial values can, however, be used based onthe structure of the optical disk 101.

When recording the first pattern signal is completed, a second patternsignal is recorded. Shown in FIG. 11 are second pattern signal 1101,which is the output signal from the pattern signal generator 125, outputsignal 1102 from the pulse generator 111, output signal 1103 from thepulse moving circuit 110; and mark pattern 1104 formed in the recordingtrack of the optical disk 101 based on output signal 1103. The firstpulse settings 5S4M and 3S5M, and last pulse settings 4M5S and 5M3S inFIG. 4(a) are then updated using the same method described above usingthe first specific pattern signal 201.

When recording the second pattern signal is completed, a third patternsignal is recorded. Shown in FIG. 12 are third pattern signal 1201,which is the output signal from the pattern signal generator 125, outputsignal 1202 from the pulse generator 111, output signal 1203 from thepulse moving circuit 110, and mark pattern 1204 formed in the recordingtrack of the optical disk 101 based on output signal 1203. In FIG. 12,the 10T period of 1210 and 1211 (a 6T space and 4T mark) and the 10Tperiod of 1212 and 1213 (a 4T mark and 6T space) have the same timelength and appear as a continuous wave. Measured signal 1210-1211 andthe next measured signal 1212-1213 therefore have the same length, andit is difficult to accurately separate and measure the measured signals.Utilizing the fact that jitter is minimized if the two 10T periods aresubstantially the same length, a jitter meter can therefore besubstituted for measurement. Other than these signal periods, the samemethod used with the first pattern is applied to set and update thefirst pulse settings 4S4M and 3S3M, and last pulse settings 4M4S and3M3S in FIG. 4(a).

When recording the third pattern signal is completed, a fourth patternsignal is recorded. Shown in FIG. 13 are fourth pattern signal 1301,which is the output signal from the pattern signal generator 125, outputsignal 1302 from the pulse generator 111, output signal 1303 from thepulse moving circuit 110, and mark pattern 1304 formed in the recordingtrack of the optical disk 101 based on output signal 1303. The firstpulse setting 4S3M and last pulse setting 4M3S in FIG. 4(a) are updatedusing the same method used with the first pattern signal.

When recording the fourth pattern signal is completed, a fifth patternsignal is recorded. Shown in FIG. 14 are fifth pattern signal 1401,which is the output signal from the pattern signal generator 125, outputsignal 1402 from the pulse generator 111, output signal 1403 from thepulse moving circuit 110, and mark pattern 1404 formed in the recordingtrack of the optical disk 101 based on output signal 1403. The firstpulse setting 3S4M and last pulse setting 3M4S in FIG. 4(a) are updatedusing the same method used with the fourth pattern signal.

It is therefore possible with the method according to this preferredembodiment to compensate during recording for the effects of heataccumulation and thermal interference during recording and distortionfrom the equalizer during reproduction, and thus record a mark/spacepattern with little jitter, by determining the mark start position fromthe length of the recorded mark and the length of the space precedingthe mark, and determining the mark end position from the length of therecorded mark and the length of the space following thereafter.

In addition, by recording first to fifth patterns and compensating themark start and end positions to minimize the offset from a specificreference edge and the normal mark length, optimum first pulse and lastpulse movement can be determined for any signal pattern not contained inthe first to fifth patterns. It is therefore possible to record marks atthe correct position during actual data recording, and recording withlittle jitter can thus be achieved.

It should also be noted that the method according to this preferredembodiment uses simple symbol patterns whereby the difference DSV iscontrolled to substantially zero only when DSV is not 0. As noted above,DSV is the difference between the reference signal, measured signal, andmarks and spaces in a specific period.

For example, the sum of marks in the first pattern signal 201 in FIG. 2is 34T and the sum of spaces is also 34T. By incorporating into onepattern two types of measured marks with different edge intervals, thesettings shown in FIG. 4(a) can be determined using fewer patterns. Itis also possible to minimize the time and recording track space, and thescale of the pattern signal generator 125, needed to determine thesettings.

As described above, the pulse position offset measuring circuit 120measures the position offset of the output signal from the digitizingcircuit 115 to detect the edge interval or jitter interval, modifies thetable stored in memory 127 based on the measured results, and sends asignal indicative of the corrected pulse edge position to the pulsemoving circuit 110 to shift the first pulse and last pulse.

It is alternatively possible, however, to pass the output signal fromthe digitizing circuit 115 over a general purpose interface bus (GPIB)to a timer interval analyzer or other analyzer for measuring the timeinterval or jitter, further connect the time interval analyzer over aGPIB to a personal computer, and then pass signals from the personalcomputer to the pulse moving circuit 110 through a SCSI or other businterface. In this case it is not necessary for the recording device tocomprise the pulse position offset measuring circuit 120, and can thusbe simplified.

It is to be noted that while this preferred embodiment shifts the firstpulse and last pulse according to the specific mark/space combination,the same method can be applied to optimize the pulse width in arecording method whereby the pulse width of the first pulse and lastpulse are modified.

FIG. 22 shows the signal parts corresponding to 6T mark 213 in firstpattern signal 201 and 6T mark 213 in pulse generator output signal 202in FIG. 2 when the space length before the 6T mark is 6T, 4T and 3Taccording to an alternative method of the present embodiment wherebyoptimization is achieved by pulse width modification.

The width of the first pulse changes according to the length of the markand the preceding space. In this preferred embodiment, both marks andspaces are separated into three groups of 3T, 4T, and 5T or longer, andthe mark edge movement is therefore defined for nine possiblecombinations of marks and spaces.

Movement of the rising edge of the first pulse is expressed as movementTF referenced to the rising edge of first pattern signal 201, forexample. The falling edge of the first pulse does not move. 6T mark 213belongs to the 5S5M group because the preceding space is 6T long, andTFI is approximately 1 ns. When the preceding space is 4T long, movementof the rising edge of the first pulse is in the 4S5M group, and TF2 isapproximately 3 ns. When the preceding space is 3T long, the first pulsewidth is in the 3S5M group, and TF3 is approximately 5 ns. Note thatwhile the value of TF changes, the falling edge of the first pulse doesnot move. As a result, the width of the first pulse changes.

FIG. 23 shows the signal parts corresponding to 6T mark 213 in firstpattern signal 201 and 6T mark 213 in pulse generator output signal 202in FIG. 2 when the space length before the 6T mark is 6T, 4T and 3Taccording to a further alternative method of the present embodimentwhereby optimization is achieved by pulse width modification.

In this case, movement of the rising edge of the last pulse is expressedas TL referenced, for example, to two clocks before the falling edge ofthe first pattern signal 201. The falling edge of the last pulse doesnot move. Because the following space is 6T long, 6T mark 213 is in the5M5S group, and TL1 is approximately 13 ns. When the following space is4T, movement of the rising edge of the last pulse is in the 5M4S group,and TL2 is approximately 11 ns. When the following space is 3T, the lastpulse width group is 5M3S, and TL3 is approximately 9 ns. Note thatwhile the value of TL changes, the rising edge of the last pulse doesnot change. As a result, the width of the last pulse changes.

It is to be noted that various methods other than changing the pulseposition or pulse width can be used for controlling the mark start andmark end positions, including adjusting the laser power at a specificpulse. Using the TF and TL value tables to achieve the intendedoptimized recording benefits of the present invention therefore requiresthat the optimization method used to correct these tables be recordedwith the tables. This can be accomplished by recording the controlmethod or by recording a predetermined code indicative of the controlmethod.

A data recording medium and optical data recording method according toalternative embodiments of the present invention are described next withreference to the accompanying diagrams. FIG. 15 is a block diagram of adata recording medium and optical data recording device according to asecond preferred embodiment of the present invention. Shown in FIG. 15are: an optical disk 1501, spindle motor 1502, semiconductor laser 1503,collimator lens 1504, beam splitter 1505, objective lens 1506,collective lens 1507, photodetector 1508, laser drive circuit 1509,pulse moving circuit 1510, delay circuits 1528 and 1529, pulse generator1511, preamp 1512, low pass filter 1513, reproduction equalizer 1514,digitizing circuit 1515, PLL 1516, demodulation and error correctioncircuit 1517, reproduction data signal 1518, power setting circuit 1519,and memory 1520.

FIG. 16 is a plan view of the optical disk 1501. In this exemplaryembodiment, the optimum position information for the mark start and endpositions, that is, the two corrected tables shown in FIG. 4(a) anddetermined as described in the first embodiment of the presentinvention, is stored in recording area 1601. These tables comprise pitand land or mark and space bit sequences printed to the insidecircumference area of the disk by the disk manufacturer prior toshipping. These two corrected tables are compiled by the manufacturer ofthe optical disk, and are prestored to every optical disk. The end-userthus obtains optical disks to which these two corrected tables havealready been stored, and uses such disks with the device shown in FIG.15.

The optical data recorder shown in FIG. 15 has an optical headcomprising semiconductor laser 1503, collimator lens 1504, beam splitter1505, objective lens 1506, collective lens 1507, and photodetector 1508.When an optical disk 1501 is loaded into this optical data recorder andthe recorder completes a specific operation for recognizing the disk,the optical head moves to the recording area 1601 storing the optimummark start and end position data tables, and reads the storedinformation. The data read from recording area 1601 thus contains theinformation compiled in the two tables shown in FIG. 4(a), and thereproduced tables are thus stored to memory 1520.

Mass manufacturing optical disks thus containing the corrected tablesdescribed above is described next.

Two corrected tables, such as shown in FIG. 4(a), are first compiled bydetermining the optimum mark start and end positions using a method suchas described in the above first exemplary embodiment of the presentinvention. The content of these tables is then recorded to the recordingarea 1601 of the optical disk 1501 using a laser to cut the informationinto the master that will be used for stamping the optical disk 1501during production when the recording area 1601 is recorded with a pitand land sequence.

FIG. 27 shows a mastering system for cutting an optical disk master.Shown in FIG. 27 are memory 2701, adjustment method data generator 2702,recording signal generator 2703, light modulator 2704, beam generator2705, lens assembly 2706, glass master 2708 coated with a photosensitivematerial 2707, turntable 2709, and motor 2710.

The two corrected tables shown in FIG. 4(a) are stored to the memory2701 in FIG. 27. Next, the method used for adjusting the first and lastpulses is output from the adjustment method data generator 2702, and thecontent of the two tables is then output from memory 2701. The recordingsignal generator 2703 then processes the adjustment method and tabledata, including modulation, adding an error correction code, scrambling,and other desired processes, and generates the two-value data used forrecording. The laser beam generated from the solid laser generator 2705,which oscillates at the wavelength of ultraviolet or the likewavelength, is power modulated by the output signal from the recordingsignal generator 2703. The modulated laser beam is fed through the lensassembly and impinges onto the photosensitive material 2707 on the glassmaster 2708. Recording the two-value signal is achieved at this time byturning the laser beam on and off to expose or not expose thephotosensitive layer appropriately. It is to be noted that the twotables stored to the memory 2701 are recorded to an area on the insidecircumference side of the user data area where the end user recordsdata, and the adjustment method data is recorded to the area to theinside circumference side of the area to which the two tables arestored.

The area exposed by an ultraviolet laser is then melted and a metalstamping master with pits and lands is produced by sputtering the glasssubstrate with nickel or metal. This metal stamping master is used as adie for producing a disk substrate on which a recording film is formed.A single disk is produced by combining two substrates, at least one ofwhich has a recording film formed thereon.

Returning to FIG. 15, the laser beam emitted from the semiconductorlaser 1503 is converted to parallel light by the collimator lens 1504,and passed to the beam splitter 1505. Light passing the beam splitter1505 is collected by the objective lens 1506, and emitted to the opticaldisk 1501 as a light spot.

Light reflected from the optical disk 1501 is then collected by theobjective lens 1506, and passed again through the beam splitter 1505.Light reflected from the beam splitter is collected by the collectivelens 1507, and focused on the photodetector 1508.

The photodetector 1508 converts the light quantity to an electricalsignal, which is amplified by the preamp 1512. The output signal fromthe preamp 1512 is then passed through the low pass filter 1513 wherebyhigh frequency signal components are blocked. The reproduction equalizer1514 then equalizes the signal, which is next binarized by thedigitizing circuit 1515 using a predetermined slice level to output asignal of 0s and 1s. The clock of the output signal from the digitizingcircuit 1515 is extracted by the PLL 1516. An output signal synchronizedto the clock is then supplied to the demodulation and error correctioncircuit 1517 for demodulation and error correction of correctable data,resulting in the reproduction signal 1518.

The reproduction signal 1518, that is, the content of the two tables andthe adjustment method information, is then stored to memory 1520. Theoptimum movement information for the mark start and end positions isthen passed over bus 1521 to the pulse moving circuit 1510.

During actual recording, the power setting circuit 1519 sets the laserdrive circuit 1509 to either peak power or bias power level. Subsequentsignal flow is described further below with reference to FIG. 17.

Shown in FIG. 17 are the data recording signal 1701 input to the pulsegenerator 1511, the output signal 1702 from the pulse generator 1511,and the output signal 1703 from the pulse moving circuit 1510. Therecording marks 1704 are formed in the recording track of the opticaldisk 1501 by modulating laser power between peak power and bias powerlevels. Note that signals 1701, 1702, and 1703 are not actually on thesame time axis, but are shown with corresponding parts alignedvertically in FIG. 17 for ease of understanding only.

In the data recording signal 1701, mark parts 1706, 1708, and 1710 arethe parts of the signal whereby a mark is formed on the disk, and spaceparts 1707, 1709, and 1711 are the parts of the signal that appear as aspace on disk.

For example, when data generated by (2,10) run-length limited modulationis recorded using a mark edge recording method, the marks and spaceshave a shortest length of 3T and a longest length of 11T where T is thereference period. Mark part 1706 is a 6T mark, space 1707 is a 6T space,1708 is a 4T mark, 1709 is a 4T space, 1710 is a 6T mark, and 1711 is a6T space.

This data recording signal 1701 is converted to a pulse sequence by thepulse generator 1511, resulting in the output signal 1702. Pulse outputfrom the pulse generator 1511 corresponding to marks of lengths 3T to11T is shown in FIG. 18.

Referring, by way of example, to a 6T signal in FIG. 18, the pulse atthe start of the signal is referred to as the first pulse 1801, and thepulse at the end of the signal is the last pulse 1804. The pulsesbetween the first pulse 1801 and last pulse 1804 are referred to asmultiple pulses 1802 and have a constant period.

In a 6T mark there are two multiple pulses 1802, in a 7T mark there arethree, and in a 5T mark there is one. It will thus be obvious that thenumber of multiple pulses 1802 between the first and last pulsesincreases by one with each 1T increase in signal length, and decreasesone with each 1T decrease in signal length. A 4T mark, thereforecomprises only the first and last pulses, and has no multiple pulses1802 therebetween. In addition, a 3T mark comprises one pulse.

It is to be noted that in this preferred embodiment the time-base lengthof the first pulse is 1.5T, the last pulse is 0.5T, and the length ofthe multiple pulses is also 0.5T. The invention shall not be so limited,however, and the length of these pulses can be varied as necessaryaccording to the structure of the optical disk 1501.

As noted above, data recording signal 1701 and output signal 1702 arenot on the same time base. However, the difference between the risingedge of the data recording signal 1701 and the rising edge of the firstpulse of the output signal 1702 is the same for any particular markparts, and the difference between the falling edge of the data recordingsignal 1701 and the falling edge of the last pulse of the output signal1702 is also the same for any particular mark parts.

The pulse generator output signal 1702 is input to the pulse movingcircuit 1510, which generates and outputs a signal 1703 in which thepositions of the first pulse and last pulse are moved. FIG. 19 shows thetables stored to memory 1520.

It is to be noted that the tables in FIG. 19 are identical to the tablesshown in FIG. 4(a), and show the combinations of marks and spaces usedfor shifting the first pulse and last pulse positions.

The position of the first pulse changes according to the length of themark and the immediately preceding space. In this preferred embodiment,the marks and spaces are separated into three groups, that is, 3T, 4T,and 5T or longer. A total of nine different last pulse positions aretherefore defined.

Movement of the last pulse position is similarly corrected. That is, thelast pulse position movement changes according to the mark length andthe length of the following space. In this exemplary embodiment marksand spaces are separated into three groups based on length, 3T, 4T, and5T or longer, and pulse position movement is defined for each of thenine possible mark/space combinations. The last pulse movement TL isthen calculated using the same method used to calculate first pulsemovement TF as described in the first embodiment.

The output signal 1703 from the pulse moving circuit 1510 is input tothe laser drive circuit 1509, which produces a laser beam at peak powerat high pulses and at bias power at low pulses in the output signal1703. The resulting sequence of marks 1704 is shown in FIG. 17.

It is therefore possible to reproduce from a predetermined area on theoptical disk and store in the optical data recorder data for changingmark start and end positions according to a data signal input to theoptical data recorder for recording. As a result, it is possible for theoptical data recorder to optimally record a signal of marks and spaceseven using optical disks having different disk structures and recordingfilms.

It is to be noted that it is not necessary to obtain the optimized markstart and end position information recorded to a particular area of thedisk for all disks. More specifically, if the variation between disks issmall, the values obtained for disks of the same structure and samerecording film composition can be recorded as typical optimized values.

Furthermore, when the optimized mark start and end position values areobtained again during actual recording to further improve jitter, thetime required for the optimization process can be reduced if typicaloptimized values are prerecorded to a particular area of the disk as inthis exemplary embodiment, and these typical values are used as defaultvalues for obtaining mark start and end position values optimized forjitter.

Furthermore, while marks and spaces are separated into three groups, 3T,4T, and 5T or longer, in this preferred embodiment, the method fordetermining these groupings is the same as in the first embodimentabove. Insofar as the optimized values for first and last pulse movementare recorded to disk, various other groupings can be used according toparticular conditions. For example, four groups, such as 3T, 4T, 5T, and6T or longer, could be alternatively used.

Tables for pulse movement groupings based on mark and space lengths of3T, 4T, 5T, and 6T or longer are shown in FIG. 24. Increasing the numberof length groups used makes it possible to more precisely control firstpulse movement and last pulse movement according to the specific symbolpattern recorded, and thus enables recording with even less jitter.

It is to be noted that this preferred embodiment of the presentinvention determines and stores optimized movement information for bothfirst and last pulses, but the invention shall not be so limited.Recording optimized movement information for only one of the pulses isstill beneficial for determining the optimum pulse movement, and makesit possible to achieve recording with little jitter.

It will also be obvious to one with ordinary skill in the related artthat while this exemplary embodiment has been described recording firstand last pulse movement information optimized for particular mark andspace combinations, a recording method whereby the pulse width of thefirst pulse and last pulse is change can be alternatively used asdescribed in the first embodiment. Optimized recording of mark and spacesequences can be achieved even with different types of optical disks,such as when the disk structure or recording film is different, byprerecording optimized pulse width information to a particular area ofthe disk.

It is to be noted that various methods other than changing the pulseposition or width can be used for controlling the mark start and endpositions, including changing laser emission power at a particularpulse. Using the TF and TL value tables to achieve the intendedoptimized recording benefits of the present invention therefore requiresthat the optimization method used to correct these tables be recordedwith the tables.

FIG. 25 is a plan view of an optical disk 2501. In this exemplaryembodiment user data is recorded to data area 2502. Informationindicative of the method used to adjust the first pulse and last pulseaccording to the input data signal is recorded to area 2503 at theinside-most circumference area of the disk using a sequence of pits andlands (marks and spaces). The optimized or typical mark start and endposition information, that is, tables such as shown in FIG. 4(a) or FIG.24, is recorded to area 2504 using a sequence of pits and lands (marksand spaces).

It is therefore possible to know, by reproducing the data stored to area2503, what method is used for adjusting the marks and spaces, that is,whether the first or last pulse is moved or whether the pulse width ischanged.

It is to be noted that variables introduced by the recording device,such as the shape of the laser spot emitted to the disk, can also causethe optimum position of the mark start and end positions required forthe best recording results to vary. To compensate for this, theoptimized or typical position information recorded to a particular areaof the disk during disk manufacture can be reproduced and these initialvalues used for a recording test whereby the position values areoptimized for the recording device.

This makes it possible to reduce the number of patterns that must berecorded to determine the optimum mark start and end positions foractual data recording. It also reduces the time required for thisoptimization procedure.

FIG. 26 is a plan view of a further optical disk 2601. In this exemplaryembodiment user data is recorded to data area 2602. Informationindicative of the method used to adjust the first pulse and last pulseaccording to the input data signal is recorded to area 2603 at theinside-most circumference area of the disk using a sequence of pits andlands (marks and spaces). The optimized or typical mark start and endposition information is recorded to area 2604 using a sequence of pitsand lands (marks and spaces). In addition, this optical disk 2601comprises a test recording area 2605.

With an optical disk 2601 thus comprised, the optimization method isread from area 2603, and the mark start and end position information isread from area 2604, and based on this information a test recording ismade in area 2605 using a method such as described in the firstembodiment of the present invention. This makes it possible to achievemore optimized recording than is possible using only the settingsprerecorded to the disk.

It should be noted that by recording the area 2503 or 2603 containingthe method used for adjusting the first pulse and last pulse to theinside circumference side of the area 2504 or 2604 to which theoptimized or typical mark start and end position information is recordedduring disk manufacture as shown in FIG. 25 or FIG. 26, respectively,the recording method can be quickly determined when reproductionproceeds from the inside circumference area of the disk, and the timerequired to complete any settings that are dependent upon the recordingmethod can be reduced.

It will also be obvious to one with ordinary skill in the related artthat while the preferred embodiments of the present invention have beendescribed above using an optical disk by way of example, the inventionshall not be so limited. More specifically, the same benefits can beachieved using a tape or card type recording medium or recording andreproducing device without departing from the scope of the accompanyingclaims.

It will thus be known from the above that an optical data recordingdevice according to the present invention records first to fifthpatterns of exemplary recording symbol sequences, and then reproducesthese patterns to determine the optimum movement of the first and lastpulses. These optimized first and/or last pulse movement values are thenrecorded to the recording medium during production. As a result, when anend user records information to the recording medium, this informationcan be reproduced to reduce or eliminate the time and effort requiredfor the recording device to learn the optimum movement information.Marks can therefore be recorded with higher precision, and recordingwith little jitter can be achieved.

Furthermore, optimized recording can be achieved even with differenttypes of optical disks, that is, optical disks having different diskstructures or recording film compositions, using a data recording mediumaccording to the present invention by recording to a particular area ofthe data recording medium information indicative of the change in themark start and end positions required for input data signals ofdifferent symbol patterns, and then reproducing and storing thisinformation in the recording device at the time of data recording.

Although the present invention has been described in connection with thepreferred embodiments thereof with reference to the accompanyingdrawings, it is to be noted that various changes and modifications willbe apparent to those skilled in the art. Such changes and modificationsare to be understood as included within the scope of the presentinvention as defined by the appended claims, unless they departtherefrom.

What is claimed is:
 1. A method for obtaining a first pulse movement TFfor a data recording medium having: a plurality of tracks; marks formedby emitting to a track in the data recording medium an optical beammodulated by one or a plurality of drive pulses where a number of thedrive pulses is determined according to a length of a mark part in theoriginal signal to be recorded to the track; a data recording area forrecording information using the marks and spaces between the marks; anda control information recording area having recorded thereto at least afirst pulse movement TF and a last pulse movement TL, whereby at least afirst pulse movement TF and a last pulse movement TL of the drive pulseis changed so as to make a reproduction jitter a specific value or less;said method comprising: generating a pattern signal containing: ameasuring signal having a mark part with a specific length of PT and aneighboring space part with a specific length of QT where T is areference period, P is a positive integer, and Q is a positive integer;and a reference signal having a mark part with a predetermined lengthand a neighboring space part with a predetermined length, said referencesignal located adjacent said measuring signal; storing the patternsignal; generating one or a plurality of drive pulses corresponding tosaid mark part of the pattern signal; forming spaces and marks on thedata recording medium by generating and emitting thereto an optical beammodulated according to the plurality of drive pulses; reproducing themarks and spaces recorded to the data recording medium to obtain areproduced pattern signal; comparing and obtaining a difference betweenthe reproduced pattern signal, and the stored pattern signal; andobtaining from this difference a first pulse movement TF for applicationto an original signal containing a sequence of space parts of length QTand mark parts of length PT.
 2. The method as set forth in claim 1,wherein said measuring signal has a mark with various lengths eachrepresenting a group of one or more mark length, and a space withvarious lengths each representing a group of one or more mark length,and wherein said reference signal has a mark length corresponding to thelength of the mark contained in a group of the longest entry in themeasuring signal and a space length corresponding to the length of thespace contained in a group of the longest entry in the measuring signal.3. The method as set forth in claim 1, wherein said first pulse movementTF is obtained for a plurality of combinations of mark lengths and spacelengths by changing P and Q.
 4. The method as set forth in claim 1,wherein the pattern signal contains an adjustment signal for obtaining aDSV of
 0. 5. A method for obtaining a last pulse movement TL for a datarecording medium having: a plurality of tracks; marks formed by emittingto a track in the data recording medium an optical beam modulated by oneof a plurality of drive pulses where a number of the drive pulses isdetermined according to a length of a mark part in the original signalto be recorded to the track; a data recording area for recordinginformation using the marks and spaces between the marks; and a controlinformation recording area having recorded thereto at least a firstpulse movement TF and a last pulse movement TL, whereby at least a firstpulse movement TF and a last pulse movement TL of the drive pulse ischanged so as to make a reproduction jitter a specific value or less;said method comprising: generating a pattern signal containing: ameasuring signal having a mark part with a specific length of PT and aneighboring space part with a specific length of QT where T is areference period, P is a positive integer, and Q is a positive integer;and a reference signal having a mark part with a predetermined lengthand a neighboring space part with a predetermined length, said referencesignal located adjacent said measuring signal; storing the patternsignal; generating one or a plurality of drive pulses corresponding tosaid mark part of the pattern signal; forming spaces and marks on thedata recording medium by generating and emitting thereto an optical beammodulated according to the plurality of drive pulses; reproducing themarks and spaces recorded to the data recording medium to obtain areproduced pattern signal; comparing and obtaining a difference betweenthe reproduced pattern signal, and the stored pattern signal; andobtaining from this difference a last pulse movement TL for applicationto an original signal containing a sequence of space parts of length QTand mark parts of length PT.
 6. The method as set forth in claim 5,wherein said measuring signal has a mark with various lengths eachrepresenting a group of one or more mark length, and a space withvarious lengths each representing a group of one or more mark length,and wherein said reference signal has a mark length corresponding to thelength of the mark contained in a group of the longest entry in themeasuring signal and a space length corresponding to the length of thespace contained in a group of the longest entry in the measuring signal.7. The method as set forth in claim 5, wherein said last pulse movementTL is obtained for a plurality of combinations of mark lengths and spacelengths by changing P and Q.
 8. The method as set forth in claim 5,wherein the pattern signal contains an adjustment signal for obtaining aDSV of
 0. 9. An apparatus for obtaining a first pulse movement TF for adata recording medium having: a plurality of tracks; marks formed byemitting to a track in the data recording medium an optical beammodulated by one or a plurality of drive pulses where a number of thedrive pulses is determined according to a length of a mark part in theoriginal signal to be recorded to the track; a data recording area forrecording information using the marks and spaces between the marks; anda control information recording area having recorded thereto at least afirst pulse movement TF and a last pulse movement TL, whereby at least afirst pulse movement TF and a last pulse movement TL of the drive pulseis changed so as to make a reproduction jitter a specific value or less;said apparatus comprising: device operable to generate a pattern signalcontaining: a measuring signal having a mark part with a specific lengthof PT and a neighboring space part with a specific length of QT where Tis a reference period, P is a positive integer, and Q is a positiveinteger; and a reference signal having a mark part with a predeterminedlength and a neighboring space part with a predetermined length, saidreference signal located adjacent said measuring signal; device operableto store the pattern signal; device operable to generate one or aplurality of drive pulses corresponding to said mark part of the patternsignal; device operable to form spaces and marks on the data recordingmedium by generating and emitting thereto an optical beam modulatedaccording to the plurality of drive pulses; device operable to reproducethe marks and spaces recorded to the data recording medium to obtain areproduced pattern signal; device operable to compare and obtain adifference between the reproduced pattern signal, and the stored patternsignal; and device operable to obtain from this difference a first pulsemovement TF for an original signal containing a sequence of space partsof length QT and mark parts of length PT.
 10. The method as set forth inclaim 9, wherein said measuring signal has a mark with various lengthseach representing a group of one or more mark length, and a space withvarious lengths each representing a group of one or more mark length,and wherein said reference signal has a mark length corresponding to thelength of the mark contained in a group of the longest entry in themeasuring signal and a space length corresponding to the length of thespace contained in a group of the longest entry in the measuring signal.11. The apparatus as set forth in claim 9, wherein the first pulsemovement TF is obtained for a plurality of combinations of mark lengthsand space lengths by changing P and Q.
 12. The apparatus as set forth inclaim 9, wherein the combinations are classified, and wherein saiddevice operable to reproduce comprises an equalizer, and the ratiobetween the output amplitude of said equalizer at the frequency of thelongest mark and the output amplitude of said equalizer at the frequencyof the shortest mark is 3 dB or less, provided that the longest mark andthe shortest mark are from the same classification.
 13. The apparatus asset forth in claim 9, wherein the pattern signal contains an adjustmentsignal for obtaining a DSV of
 0. 14. An apparatus for obtaining a lastpulse movement TL for a data recording medium having: a plurality oftracks; marks formed by emitting to a track in the data recording mediuman optical beam modulated by one or a plurality of drive pulses where anumber of the drive pulses is determined according to a length of a markpart in the original signal to be recorded to the track; a datarecording area for recording information using the marks and spacesbetween the marks; and a control information recording area havingrecorded thereto at least a first pulse movement TF and a last pulsemovement TL, whereby at least a first pulse movement TF and a last pulsemovement TL of the drive pulse is changed so as to make a reproductionjitter a specific value or less; said apparatus comprising: deviceoperable to generate a pattern signal containing: a measuring signalhaving a mark part with a specific length of PT and a neighboring spacepart with a specific length of QT where T is a reference period, P is apositive integer, and Q is a positive integer; and a reference signalhaving a mark part with a predetermined length and a neighboring spacepart with a predetermined length, said reference signal located adjacentsaid measuring signal; device operable to store the pattern signal;device operable to generate one or a plurality of drive pulsescorresponding to said mark part of the pattern signal; device operableto form spaces and marks on the data recording medium by generating andemitting thereto an optical beam modulated according to the plurality ofdrive pulses; device operable to reproduce the marks and spaces recordedto the data recording medium to obtain a reproduced pattern signal;device operable to compare and obtain a difference between thereproduced pattern signal, and the stored pattern signal; and deviceoperable to obtain from this difference a last pulse movement TL for anoriginal signal containing a sequence of space parts of length QT andmark parts of length PT, and storing last pulse movement TL.
 15. Themethod as set forth in claim 14, wherein said measuring signal has amark with various lengths each representing a group of one or more marklength, and a space with various lengths each representing a group ofone or more mark length, and wherein said reference signal has a marklength corresponding to the length of the mark contained in a group ofthe longest entry in the measuring signal and a space lengthcorresponding to the length of the space contained in a group of thelongest entry in the measuring signal.
 16. The apparatus as set forth inclaim 14, wherein said first pulse movement TF is obtained for aplurality of combinations of mark lengths and space lengths by changingP and Q.
 17. The apparatus as set forth in claim 14, wherein thecombinations are classified, and wherein said device operable toreproduce comprises an equalizer, and the ratio between the outputamplitude of said equalizer at the frequency of the longest mark and theoutput amplitude of said equalizer at the frequency of the shortest markis 3 dB or less, provided that the longest mark and the shortest markare from the same classification.
 18. The apparatus as set forth inclaim 14, wherein the pattern signal contains an adjustment signal forobtaining a DSV of 0.